CN106471340A - For the device from multiple fiber sensor measuring optical signals - Google Patents
For the device from multiple fiber sensor measuring optical signals Download PDFInfo
- Publication number
- CN106471340A CN106471340A CN201580030292.6A CN201580030292A CN106471340A CN 106471340 A CN106471340 A CN 106471340A CN 201580030292 A CN201580030292 A CN 201580030292A CN 106471340 A CN106471340 A CN 106471340A
- Authority
- CN
- China
- Prior art keywords
- fbg
- array
- pulse
- wavelength
- light source
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000003287 optical effect Effects 0.000 title claims description 63
- 239000000835 fiber Substances 0.000 title claims description 35
- 239000013307 optical fiber Substances 0.000 claims abstract description 69
- 238000000985 reflectance spectrum Methods 0.000 claims abstract description 41
- 238000001228 spectrum Methods 0.000 claims description 73
- 238000000034 method Methods 0.000 claims description 36
- 238000005259 measurement Methods 0.000 claims description 31
- 230000011664 signaling Effects 0.000 claims description 31
- 230000003595 spectral effect Effects 0.000 claims description 23
- 230000008859 change Effects 0.000 claims description 15
- 238000001816 cooling Methods 0.000 claims description 11
- 238000003491 array Methods 0.000 claims description 10
- 230000004044 response Effects 0.000 claims description 10
- 230000008569 process Effects 0.000 claims description 8
- 238000012544 monitoring process Methods 0.000 claims description 6
- 230000006978 adaptation Effects 0.000 claims description 5
- 238000001514 detection method Methods 0.000 claims description 5
- 238000012545 processing Methods 0.000 claims description 5
- 230000005619 thermoelectricity Effects 0.000 claims description 4
- 230000000694 effects Effects 0.000 claims description 3
- 230000003993 interaction Effects 0.000 claims description 3
- 238000004891 communication Methods 0.000 claims description 2
- 230000008034 disappearance Effects 0.000 claims description 2
- 230000007774 longterm Effects 0.000 claims description 2
- 238000000691 measurement method Methods 0.000 claims 1
- 230000006870 function Effects 0.000 description 12
- 238000004080 punching Methods 0.000 description 9
- 210000003462 vein Anatomy 0.000 description 9
- 210000001367 artery Anatomy 0.000 description 8
- 230000008901 benefit Effects 0.000 description 8
- 238000009826 distribution Methods 0.000 description 6
- 238000005516 engineering process Methods 0.000 description 6
- 238000009434 installation Methods 0.000 description 5
- 238000002310 reflectometry Methods 0.000 description 5
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 238000013461 design Methods 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 238000006243 chemical reaction Methods 0.000 description 2
- 239000000284 extract Substances 0.000 description 2
- 238000012886 linear function Methods 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 230000000149 penetrating effect Effects 0.000 description 2
- 230000005622 photoelectricity Effects 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 230000003321 amplification Effects 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000000903 blocking effect Effects 0.000 description 1
- 238000011088 calibration curve Methods 0.000 description 1
- 230000000747 cardiac effect Effects 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 238000012217 deletion Methods 0.000 description 1
- 230000037430 deletion Effects 0.000 description 1
- 230000004069 differentiation Effects 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 238000000855 fermentation Methods 0.000 description 1
- 230000004151 fermentation Effects 0.000 description 1
- 230000036039 immunity Effects 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 230000002045 lasting effect Effects 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004899 motility Effects 0.000 description 1
- 238000010606 normalization Methods 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 230000002085 persistent effect Effects 0.000 description 1
- 230000000644 propagated effect Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 238000005057 refrigeration Methods 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 238000012732 spatial analysis Methods 0.000 description 1
- 238000003786 synthesis reaction Methods 0.000 description 1
- 230000036327 taste response Effects 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
- 238000004148 unit process Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
- G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
- G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
- G01D5/35338—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using other arrangements than interferometer arrangements
- G01D5/35354—Sensor working in reflection
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
- G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
- G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
- G01D5/35383—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using multiple sensor devices using multiplexing techniques
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/02—Details
- G01J3/0205—Optical elements not provided otherwise, e.g. optical manifolds, diffusers, windows
- G01J3/0218—Optical elements not provided otherwise, e.g. optical manifolds, diffusers, windows using optical fibers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/28—Investigating the spectrum
- G01J3/45—Interferometric spectrometry
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/12—Generating the spectrum; Monochromators
- G01J3/18—Generating the spectrum; Monochromators using diffraction elements, e.g. grating
- G01J3/1895—Generating the spectrum; Monochromators using diffraction elements, e.g. grating using fiber Bragg gratings or gratings integrated in a waveguide
Landscapes
- Physics & Mathematics (AREA)
- Spectroscopy & Molecular Physics (AREA)
- General Physics & Mathematics (AREA)
- Optical Transform (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Measuring Temperature Or Quantity Of Heat (AREA)
Abstract
This invention describes a sensor device.This device includes interrogator, and interrogator includes launching the light source with certain wavelength, and certain wavelength is about a mean wavelength;Configure with a Fiber Bragg Grating FBG (FBG).This configuration includes FBG array, and this array includes multiple multiple FBG in an optical fiber and is used for reflected impulse, produces reflected impulse therefore on each FBG.FBG on one given FBG array therebetween has a space interval, and this interval allows to be formed between the reflected impulse that each sensor produces on a sensor time difference.Described FBG array has a reflectance spectrum window, and this reflectance spectrum window includes mean wavelength.
Description
To Cross-Reference to Related Applications
This application claims the priority of the U.S. Provisional Application in April 2 Application No. in 2014 " 61/973,975 "
Background
(a) technical field
Disclosed theme is usually directed to fibre opticss, more properly, the present invention relates to fiber Bragg grating sensor.
(b) background technology
Fiber Bragg Grating FBG (FBGs) has been found to be the efficient apparatus for monitoring physical parameter, physical parameter includes
But it is not limited to, temperature, strain, pressure, vibration.FBG passes through the core of one optical fiber in given length (typically several millimeters)
Permanent cycle variations in refractive index and manufacture.This equipment reflects to be propagated by the light of narrow wave-length coverage in a fiber.Instead
Penetrating spectrum generally has a narrow peak value in wavelengths centered, and the screen periods that narrow peak value is equal in space are multiplied by the two of fiber refractive index
Times.The width of reflectance spectrum and grating length are inversely proportional to.In order to FBG is used as sensor, conversion configurations are to the light comprising grating
Fine change temperature or stretching section, both effects lead to the change of grating effective period, thus leading to reflect center wavelength of light
Change.Therefore, the measurement of this centre wavelength can be associated with measured parameter (measured variable).Can be by emitting light into
In the optical fiber of distant place, detect and analyze the spectral characteristic of reflected light and remotely measure.Because fibre loss is very low, measurement sets
The standby position being placed on away from FBG.
FBG is optical fiber immunity electromagnetic interference so that they are possible to be applied to electricity as an advantage of sensing device
In the environment of sensor or electronic sensor can not well execute.
But one of major advantage of FBG is, due to their narrow spectral characteristic, multiple FBG of different cycles are permissible
It is written into the diverse location of a single optical fiber, and each FBG can be identified by spectral characteristic.And with individually
A piece optical fiber, multiple locus can be sensed by measuring the peak wavelength of FBG simultaneously.Along an optical fiber, by multiple FBG
The technology that sensor is combined from different centre wavelengths is referred to as wavelength-division multiplex (Wavelength Division
), or WDM Multiplexing.
The method being commonly used for monitoring the centre wavelength of FBG is tunable with multiple scanning width wave-length coverage
Light source.Reflected light is collected by the optical circulator being arranged between light source and FBG or photo-coupler, is subsequently sent to photodetection
On device.Peak value therefore in reflected light corresponds to each FBG peak reflectance wavelength.Or it is also possible to broadband light source, will own
The centre wavelength of FBG falls into source spectrum.Then reflected light is sent to spectrogrph, is determined by analyzing spectrogrph data
Reflection peak.
For WDM inquiry, all FBG along optical fiber have the light in tunable optical source or broadband light source
There is centre wavelength in spectral limit.On the other hand, the wavelength spacing of each FBG must sufficiently large be affected with being contained in measured parameter
The maximum spectral shift of each FBG lower, not have the probability of overlap between each spectrum, overlap will lead to fuzzy or mistake
Measurement.One " spectrum window " (spectral window) therefore can be defined, that is, give under measured variable scope, FBG senses
The centre wavelength scope that device may span across.As a result, the maximum quantity of the FBG that can be inquired by given light source, about etc.
In spectral width or light source span divided by the spectrum window of separated sensor spectral width.
For example, the centre wavelength of typical FBG is in proportional shifting for strain, therefore, if strain that will be measured
Up to 10,000 μ ε, then 10nm is approximated for a FBG maximum wavelength skew with 1550nm centre wavelength.If can
Tuning source has the scope of 60nm, as typical commercial source, then the maximum quantity that can use the sensor in this source is 6, by
Given 60nm is given divided by the 10nm of spectrum window.
Some applications will benefit because carrying greater number of sensor on same fiber.For example, for equipment part,
For example, the temperature of the spatial analysis of the equipment part of wind turbine blade machine or generator amature or strain, it will benefit from
There is the number of sensors of 100 or bigger scope.
A method increasing number of sensors is come distinguishing sensor with time domain and wavelength category.This scheme is labeled
For time division multiplexing (Time-division-multiplexing), or TDM, in TDM scheme, for inquiring the light of grating
Source is pulse modulated, and the pulse duration is set as being shorter than the optical path delay from a grating to next grating.If
The maximum reflectivity of each grating is sufficiently small (typically 1%-2%), then the first reflection being only from each grating is aobvious
Write, and the signal that on grating reflector, the light of multiple reflections reflects is negligible.Therefore each pulses generation is a series of
Echo, echo can be distinguished in time.As WDM inquiry scheme, source can be tunable or wide band.Different
Part is, detection means must have response time, and response time will the short enough reflection being come from numerous gratings with differentiation.Cause
This, multiple FBG can be used in single spectrum window.Therefore, the sum that the sum of sensor configures for WDM is multiplied by can quilt
The quantity of the sensor of timing separation.
Although this combination TDM-WDM inquiry scheme can use tunable source, the prior art that major part refers to
Using broadband light source.Because broadband light source has there are all wavelengths for inquiring sensor in all times, this meaning
Taste response time and is not limited by source.Tunable source always needs the whole span lengths of some time sweeps, and this time is
Limit system response time eventually.
When using wide frequency light source, the centre wavelength of grating sensor is many times passed through with spectrum sensitivity filter (example
As non-equilibrium interferometer) or radiological unit process reflected light determination.
Describe the prior art of TDM and WDM sensing device, including patent publication No. WO2013001268,
CA2379900A1, US20100128258, WO2004056017, these patents all using broadband light source and various are configured to
Gate (gate) reflected signal simultaneously detects their wavelength.
Niu Weizhasi (Niewczas) (WO2013001268A2) describes one kind broadband light source and interferometer measurement
The system of reflected light wavelength.Cooper and Smith (CA2379900A1) also using pulse modulated broadband light source and
Photomodulator gates (gate) reflected impulse.Wo Lantan and Li Aode (Volanthen and Lloyd) (US20100128258)
Also using pulse broadband source.
Ai Waao and Li Aode (Everall and Lloyd) (WO2004056017) describes one kind with by semiconductor light
Learn amplifier impulse modulation and the TDM system of gate broadband light source.With light filter known to propagation performance, or alternatively select
Spectroanalysis instrument, band meter just can determine that wavelength.The application of semiconductor optical amplifier result in bigger optical power simultaneously
(optical power), the synthesis cost of source, image intensifer and wavelength measuring equipment is still important.
When using broadband light source, a difficult point is that optical power can be assigned to whole light source spectrally.Cause
This, the actual power being reflected by each FBG is only the sub-fraction of total source power.It is true that the major part of source power
It is wasted, because it is not reflected by any sensor.Typical broadband light source, for example, light emitting diode or super spoke
Penetrate light emitting diode after being coupled into single-mode fiber, only the power of 1mW.The low-power of reflected signal is difficult to obtain one enough
Big signal to noise ratio.It is that the quantity composing window nevertheless suffers from the restriction of the total spectrum width in source using another difficult point of broadband light source.
Sum it up, most prior art is limited by extra defect, system cost.Image intensifer, fibre optic interferometer
Or spectroanalysis instrument is all comparatively expensive device.At present, the high cost of these systems hinders their extensive application.Impact sets
Another factor of standby expense is, this is an all-or-nothing apparatus.The meaning is, this apparatus energy under given cost
Enough measure substantial amounts of grating, but if the capacity that the quantity of required sensor is less than final apparatus cannot reduce payment.
It is therefore desirable to improvement fibre-optical sensing device.
Content of the invention
According to an aspect of the invention, it is provided a kind of sensor device, including:Interrogator, including light source, each light
Source transmitting has the pulse of certain wavelength, and described wavelength is around the corresponding mean wavelength of light source each described;With FBG battle array
Row, one of corresponding described light source of each FBG array, and include multiple on an optical fiber for reflected impulse
FBG, the FBG in wherein given FBG array therebetween has a space interval, and this interval be enough to
Allow on receptor to be produced the time difference between reflected impulse by each sensor on given FBG array;Wherein
Each described FBG has corresponding spectral reflectance window, and spectral reflectance window includes putting down accordingly of a corresponding described light source
All wavelength;There is spectrum interval it is sufficient to allow on the receiver from described in each between the corresponding mean wavelength of wherein said light source
SPECTRAL DIVERSITY between the pulse of FBG array reflection.
According to an embodiment, each described light source is configured to around the corresponding mean wavelength of each in described light source
First respective wavelength and the transmitting pulse of the second respective wavelength.
According to an embodiment, described receptor includes processor, and described processor is applied to each described light source corresponding
Each described FBG array, and the prior art of the reference reflectance spectrum based on each FBG, with being derived from
The reflected wave pulses of the first corresponding pulses and the second corresponding pulses clearly determine the actual reflectance spectrum of each FBG
Peakdeviation.
According to an embodiment, described FBG array is arranged on multiple optical fiber, each optical fiber have one to
The FBG array of fixed number amount.
According to an embodiment, also include the multiplexer for being connected thereto multiple optical fiber, described interrogator
It is optically coupled to multiplexer to be used for described pulsing to multiple optical fiber.
A kind of another fermentation according to the present invention, there is provided sensor device, including:Interrogator, has certain including transmitting
The light source of the pulse of individual wavelength, described wavelength is around a mean wavelength;Configure with Fiber Bragg Grating FBG (FBG), including FBG
Sensor array, described sensor array includes the multiple FBG on an optical fiber, and is used for reflected impulse, thus
Reflected impulse is produced on each FBG, the FBG on one of given FBG array betwixt has
One space interval, this space interval be enough to allow to be produced between reflected impulse by FBG each described on the receiver
Time difference;Wherein FBG array has the spectral reflectance window including described mean wavelength.
According to an embodiment, described light source is used for being transmitted in the arteries and veins of first wave length and second wave length near mean wavelength
Punching.
According to an embodiment, described receptor includes a processor, and described processor is based on described multiple FBG sensings
The prior art of the reference reflectance spectrum of device, adaptation is with the reflection arteries and veins from the first corresponding wavelength and the second corresponding wavelength
Punching clearly determines the actual reflectance spectrum of each of multiple FBG.
According to a further aspect in the invention, there is provided one kind is joined with Fiber Bragg Grating FBG (FBG) sensor for measurement
Put the device of the optical signalling of interaction, described device includes:FBG array, sensor array sets along single optical fiber
Put, each FBG is used for operating in given spectrum window, and FBG is separated along single optical fiber with given distance, in array
On each FBG have a known reflectance spectrum, this reflectance spectrum can be displaced under prescribed conditions reality anti-
Penetrate spectrally, thus defining a side-play amount;And interrogator, described interrogator is connected on single optical fiber and comprises mould
Block, the described module discrete wavelength inquiry FBG array more than being included in given spectrum window, interrogator receives
The reflection of the optical signal of the discrete wavelength more than of FBG, inclined with each FBG on array for the determination
Shifting amount.
According to an embodiment, described module is with being included in two discrete wavelength interrogation FBG in given spectrum window
Array.
According to an embodiment, the described given distance that FBG is spaced, lead to the optics being received by described interrogator
Time difference between the reflection of signal.
According to an embodiment, also include a processor, described processor is operably connected to interrogator, and is adapted to
Execute instruction is used for determining the instruction of specified criteria, under to described fixed condition it is known that reflectance spectrum be displaced on array
In the actual reflectance spectrum of each FBG.
Another invention according to the present invention, there is provided one kind is joined with Fiber Bragg Grating FBG (FBG) sensor for measurement
Put the device of the optical signalling of interaction, described device includes:Multiple FBG tactility apparatus arrays, sensor array is along in key light
Multiple optical fiber settings that fibre branches out, each of the plurality of array has different spectrum windows and includes in difference spectrum window
The FBG of operation, described FBG has a known reflectance spectrum, and this spectrum can experience in specified criteria partially
Move, therefore side-play amount is defined to each FBG;Interrogator, is connected on main fiber and includes multiple modules, each module
With a FBG corresponding more than the pulse interrogation of in the different spectrum windows of an array of corresponding FBG
Array, interrogator receives the optical signalling of the side-play amount being reflected and indicated by FBG each FBG.
According to an embodiment, each module is using the different spectrum windows in the array of corresponding FBG more than one
Pulse, the corresponding array inquiring corresponding FBG of inquiry, anti-clearly to evaluate known to each FBG
Penetrate the side-play amount of spectrum.
According to an embodiment, the FBG of described given array is separated along one of multiple optical fiber with given distance,
On optical fiber, FBG is configured to:When optical signalling is reflected by FBG, described optical signalling pulse can be produced
Time difference.
According to an embodiment, also include a multiplexer, be arranged between interrogator and multiple array, multiplexing
Device is used for for the output of multiple modules integrating with main fiber.
According to a further aspect in the invention, one kind is provided to be used for measuring Fiber Bragg Grating FBG (FBG) sensor configuration
The device of optical signalling, described device includes:Along the array of the FBG of single optical fiber setting, each described FBG
There is the known reflectance spectrum being centered around the peak reflectance wavelength of movement under change condition:And interrogator, described interrogator connection
In independent optical fiber and include:Module, be adapted to using optical signalling inquire FBG array, described optical signalling with
First wave length (λ+) or second wave length (λ-) transmitting pulse;And receptor, adaptation is to detect the arteries and veins being reflected by FBG array
Punching, i.e. reflected impulse, for determining the side-play amount of the peak reflectance wavelength at least one FBG.
According to an embodiment, also include being arranged at the array of the additional FBG of additional optical fiber, each adds
The array of FBG has different and unique peak reflectance wavelength;Described interrogator also includes additional module, adaptation
Become the array of the FBG additional with different optical signalling inquiries, described optical signalling is included with first wave length (λ+) or the
Two wavelength (λ-) pulse launched, wherein λ+And λ-It is different and unique for each additional module.
According to an embodiment, described receptor includes a photodiode, for optical signalling is changed into representative
The electronic signal of described optical signalling.
According to an embodiment, described receptor includes an amplifier and is used for amplifying described electronic signal.
According to an embodiment, described receptor is used for the processing meanss with the electronic signal processing described receptor output
Operation communication.
According to an embodiment, based on the side-play amount of peak reflectance wavelength, processor is adapted to defeated by locating reason receptor
The electronic signal going out to determine act on measured at least one FBG.
According to an embodiment, described processing equipment is adapted to acting on the temperature at least one sensor for determining
At least one of degree and strain.
According to an embodiment, also include swivel joint, described swivel joint is arranged at interrogator and described single
Between optical fiber, it is used for making single optical fiber rotate with respect to described interrogator.
According to an embodiment, described interrogator includes light source, and light source includes laser diode.
According to an embodiment it is characterised in that also including cooling element, for keeping the temperature of described light source.
According to an embodiment, described cooling unit includes the cooling unit of thermoelectricity.
According to an embodiment, also include temperature sensor, for measuring the temperature of light source, and and then notify described cold
But whether element is necessary to cool down described light source.
According to an embodiment, also include the reference laser diode for monitoring described optical signal.
According to an embodiment, described reference laser diode is the long-term wave length shift in order to monitor described light source.
According to an embodiment, also include photo-coupler, for the pulse steering of launching slave module to FBG device
And reflected impulse is configured (or FBG device) (FBG sensor arrangement) from described FBG draw
Lead described receptor, described photo-coupler has the second branch, wherein said reference photodiode is arranged on institute
State in the second branch of photo-coupler.
According to an embodiment, also include photo-coupler, for pulse steering that will launch from described module to described FBG
Sensor configuration, and described reflected impulse is directed to described receptor from the configuration of described FBG.
According to a further aspect in the invention, provide a kind of for measurement by include FBG Fiber Bragg Grating FBG
(FBG) method of the optical signalling of sensing device reflection, the method comprising the steps of:Pass to described FBG from a light source
Sensor configuration sends:At least one pulse in first wave length;With at least one pulse in second wave length, each pulse is at least
Separated with time interval T, each pulse is shorter than unit interval T, for distinguishing the reflected impulse from each FBG;
For at least one FBG, receive and measure following intensity:Reflection arteries and veins at least one pulse of first wave length
Punching;With the reflected impulse of at least one pulse in second wave length, calculate the peak reflection ripple of at least one described FBG
Long.
According to an embodiment, executed by receptor and receive and measurement intensity.
According to an embodiment, described receptor is adapted to sufficiently fast response and is derived from each sensor so that distinguishing
Reflected impulse.
According to an embodiment, described time interval T be from adjacent FBG reflected impulse in described receptor
On the time interval that received.
According to an embodiment, also include determining the reference value with respect to described peak reflectance wavelength for the described peak reflectance wavelength
Side-play amount.
According to an embodiment, also include going determination to act at least one FBG with the side-play amount of described peak reflectance wavelength
The value of the measured variable of sensor.
According to an embodiment, also include the wavelength with light source described in reference laser diode monitor.
According to an embodiment, also include the temperature using independent temperature sensor measurement reference laser diode.
According to an embodiment, also include controlling the temperature of described light source.
According to an embodiment, the temperature of light source is controlled to include:With the described light source of the cooling element cooling of thermoelectricity.
According to an embodiment, the temperature controlling light source is based on the input from temperature sensor, and described temperature sensor is surveyed
Whether the temperature of amount light source deviates particular value.
According to an embodiment, it is sent at least one pulse of first wave length with the first intensity, is sent in the second intensity
At least one pulse of second wave length, the intensity of wherein measurement reflected impulse includes detecting the disappearance of each pulse respective strengths.
According to an embodiment, configure transmission pulse to described FBG and include passing to the FBG being arranged on multiple optical fiber
Sensor sends.
According to a further aspect in the invention, provide a kind of Fiber Bragg Grating FBG comprising FBG for inquiry
(FBG) method of sensing configuration, the method comprising the steps of:Send multiple light letters to the FBG array of FBG configuration
Number, each described optical signal is used for interacting with the described FBG on single FBG array, and each optical signal includes:Accordingly
First wave length at least one pulse;With at least one pulse of corresponding second wave length, each described optical signals phase
The mean wavelength answered is to characterize, and in each optical signal described, corresponding first and second wavelength provide around described mean wavelength:
For at least one FBG of FBG array, receive and measure following intensity:At least one arteries and veins in described first wave length
The reflected impulse of punching;Reflected impulse with least one pulse in described second pulse;And FBG at least one described is passed
Sensor, calculates peak reflectance wavelength.
According to an embodiment, to each optical signal, each pulse is at least spaced corresponding time interval T, wherein each arteries and veins
Punching is shorter than corresponding time interval T.
According to an embodiment, executed by receptor and receive and measurement intensity, described receptor response sufficiently fast with can
Distinguish the reflected impulse from each FBG.
According to an embodiment, each FBG array has following characteristics:All FBG sensings of setting on each FBG array
Corresponding spectrum window shared by device, and each FBG array is inquired with a corresponding optical signalling.
According to an embodiment, between the corresponding mean wavelength of each described optical signalling, exist more than each FBG battle array
The corresponding spectrum composing window of row separates, enabling carry out spectrum difference to each FBG array.
Brief description
Combining accompanying drawing according to following detailed descriptions can be it will be apparent that shows the further feature and advantage of disclosure, its
In:
Figure 1A illustrates that an embodiment includes inquiring the single mould of the serial array of the FBG along single optical fiber setting
The installation drawing of block;
Figure 1A illustrates that an embodiment includes inquiring the single mould of the parallel array of the FBG along multiple fiber distribution
The installation drawing of block;
Fig. 2A illustrates that an embodiment includes inquiring the many of multiple serial array of the FBG along multiple fiber distribution
The installation drawing of individual module;
Fig. 2 B illustrates to comprise in an embodiment to inquire the many of multiple parallel arrays of the FBG along multiple fiber distribution
The installation drawing of individual module;
Fig. 3 A to Fig. 3 C illustrates to launch the intensity with respect to the time with reflected impulse in an embodiment;
Fig. 4 A-4C illustrates the transmitting with respect to the time in another embodiment and the intensity of reflected impulse;
Fig. 5 A and Fig. 5 B illustrates the exemplary plot of a FBG reflectance spectrum;With
Fig. 6 A-6C is the installation drawing of the photodiode of the pulse illustrating that an embodiment is included for detection transmitting;
Fig. 7 a-7C is the figure of the various embodiments of output FBG array configuration;With
Fig. 8 is to illustrate to add in an embodiment/remove how multiplexer is transmitted into detached point from one or more modules
Among figure;
It should be noted that in all of the figs, identical feature is indicated by the same numbers.
Specific embodiment
Disclosure is related to the device with reference to the multiple FBG of WDM and TDM commercial measurement.
Existing description describes the embodiment based on modular system, wherein each module low cost, building block system
Become.And, user can build an instrument by the cost proportional to the quantity of required sensor.Additionally, modularity collection
The standardization closing part allows the reduction of manufacturing cost.
The technology of the measurement FBG wavelength describing in this respect is fundamentally different from known prior art.To the greatest extent
Pipe major part prior art is intended to find the wavelength of the peak reflectivity of grating, but this description content has used FBG to compose profile
Knowledge determines the position with respect to inquiry source for the FBG centre wavelength of setted wavelength.
Referring now to Figure 1A, an equipment 1 is shown, including along single optical fiber 30 or multiple along branch out from main fiber
Multiple FBG 50 (referring to Figure 1B, 2A and 2B) of optical fiber 30 distribution, multiple FBG 50 are included into one or many
In individual sensor array 55.Each sensor array 55 is made up of N number of FBG array 50 of operation in same spectrum window, FBG
Sensor along optical fiber 30 with away from source orientation or non-directional but known distance is separated, as shown in Figure 1A.Each sensing
Device array 55 operates in different spectrum windows.Due to from all FBG 50 in array 55 all on same optical fiber 30,
Array 55 can be defined as serial array, and this is different from parallel connected array hereinafter described.
Shown in another embodiment as shown in Figure 1B, each sensor array 55 includes being distributed in multiple optical fiber 30
FBG 50, is defined as parallel connected array.Each parallel connected array is arranged on by a single optical fiber by N number of (N=4 in Figure 1B)
Sensor composition on each optical fiber that branch goes out, and be located at away from the distance of increment in source.This increment can rule can be irregular
But it is known.Fig. 2 B applies for identical principle, in Fig. 2 B, has used multiple modules, as mentioned below.
Equipment 1 also includes:Including the interrogator 12 of one or more single modules 10, each module 10 is inquired at one
One of sensor array 55 of the FBG of operation in spectrum window;If employing the module 10 (see Fig. 2) more than 1,
The output of multiple modules is incorporated in an independent optical fiber 30 optical WDM device 60;Optional spectrum adds/deletes multichannel
The output of multiple modules 10 can be segregated into each branch of optical fiber from main fiber 30 by multiplexer 65, often next passage, or
Multiple passages (see Fig. 2) every time;One or more optional reference FBG on each sensor array 55 (does not show
Go out), such a have known strained and temperature with reference to FBG.
The base unit of equipment 1 includes single module 10, in inquiry same spectrum window of positioning along in an independent optical fiber 30
One sensor array 55 with N number of FBG 50 of operation, as described in Figure 1A.As described below, to embodiment, can use
Reference photodiode does the configuration substituting, and sees Fig. 6 A-6C.By with wavelength division multiplexer their output of multichannel sender, many
Individual module 10 also can use, as shown in Figure 2 simultaneously.
Each module 10 is made up of the light source with narrow spectrum width (typically less than 1GHz), when light source is used for repeatedly launching lasting
Between be τpPulse, make τpIt is shorter than in sensor array 55 light between continuous FBG 50 and propagate minimum time τ.Transmitting pulse
Centre wavelength be forced in high numerical value λ+With low numerical value λ-Between alternately, λ+And λ-Difference more much smaller than the spectrum width of FBG 50
(such wavelength X+And λ-Pulse can be reflected by FBG), but be typically larger than spectrum width (such wavelength of each pulse
λ+And λ-Pulse can be distinguished by spectrum).Therefore one mean wavelength λ of definableav=(λ++λ-)/2, λ+、λ-And λavAll should to the greatest extent may be used
Can keep constant.
Alternate λ+And λ-Can be executed by different modes, in a kind of executive mode, as shown in Figure 3A, pulse with when
Between interval T be issued, such T be more than in sensor array first light and the FBG of last between propagate total
Time, and in λ+And λ-Between alternately.
(not shown) in another executive mode, to be spaced the λ of T transmitting+A large amount of trains of pulse follow in λ-A large amount of pulses
After string.
The third possible executive mode, shown in Fig. 4 A, launches two pulses, a λ in time interval τ+Followed by one
Individual λ-.For the third executive mode.τpIt is necessarily less than τ/2, two pulses can be different but it is also possible to be dissolved into respectively
In the first half and the second half, there is mean wavelength λ+And λ-Independent pulse in (that is, initial wavelength begins to λ+, terminate close
λ-).For reaching optimum efficiency, λ+And λ-Time between time between pulse or train of pulse is shorter than measured variable with meaningful
Numerical value change the required time.
Light pulse is launched in an optical fiber 30, and according to an embodiment, light source 11 is a kind of by alternately high and low peak
The fine coupling of electric light, the DFB laser diode (as the LD of Fig. 1) of temperature constant that the current impulse of electric current is ordered about.It is known that
The center wavelength of light of such a DFB laser diode transmitting is related to driving current, therefore has the arteries and veins of different peak point currents
Punching has different centre wavelengths.DFB laser diode module generally comprises one and is used for blocking reflected light return laser light diode
Optical isolator and monitoring be launched light inside photodiode.
Behind optical coupling source, insert fiber coupler 15 or optical circulator.This allows reflected light to be redirected to photodetection
On device 20 (PD in Fig. 1).Various other fiber arrays (in Fig. 1, C is used as general symbol(s)) can be inserted into fiber coupler 15 He
Between sensor array 55, such as wavelength division multiplexer 60, adapter, optical fiber rotary joint 70 and interpolation/deletion multiplexer
65 (as shown in Figure 2).
If substituting circulator using fiber coupler 15, the second branch of fiber coupler 15 may comprise a reference
FBG, as described below.
N number of FBG 50 of composition sensor array 55 is to have the grating Bragg falling into spectrum window internal reflection spectrum
Optical fiber 50, spectral window is defined as the wave-length coverage that wavelength in the middle of FBG covers the scope of possible numerical value exceeding measured variable.
Pulse λavMean wavelength more or less be located at spectrum window center.As in other TDM schemes, the maximum of FBG 50 is anti-
Penetrate rate must sufficiently small (be led to by more than one sensor reflection) so that multipath reflection to be ignored.Generally, this
Mean maximum reflectivity in the range of 1-2%.Therefore FBG 50 reflection light pulse, but each sensor is anti-
Rate of penetrating depends on the numerical value in each sensing station for the measured variable, because measured variable affects the middle cardiac wave of FBG reflectance spectrum
Long.Different wave length λ+And λ-Pulse also react varying strength, because their wavelength are in the diverse location of FBG reflectance spectrum.This from
Can embody in Fig. 5 A and 5B, for two λ of different numerical valueBFBG spectrum, and λ+、λ-And λavPosition in FBG spectrum,
With corresponding reflectance.
The pulse that each is launched, reflected signal be present in a series of have be equal to each FBG 50 light propagate
In N number of pulse of interpulse delays time τ of time, N is the quantity of sensor in sensor array.Because delay time T is total
It is to be longer than τp(pulse duration), therefore reflected impulse time upper difference.This shown in Fig. 3 A-3C, in one case,
Pulse to each being launched as shown in Figure 3A, it will have the such reflection in 4 shown in Fig. 3 B (N=4), wavelength will be from
Pulse is to pulse (λ+, λ-) alternately, peak strength (I simultaneously+, I-) alternately.Alternate λ is illustrated in the form of Fig. 4 A+And λ-Arteries and veins
The pattern of punching, pulse also has different peak strengths, this be likely to be using have the DFB laser diode of different peak point currents with
Change pulse wavelength.Fig. 3 B show is along the echo in the case of the array of 4 FBG of fiber distribution.
When launching two pulses in time τ, as described in Figure 4, echo is corresponding pulse pair, such as Fig. 4 B
Shown.
The echo coming from N number of FBG 50 passes through fiber coupler 15 or circulator, and is redirected to photoelectricity
On detector 20, wherein optical signal is converted to the signal of telecommunication.The response time of photoelectric detector 20 and electronic amplification circuit 25 should
It is shorter than the pulse duration so that the electronic signal amplified is the loyal time reproduction of optical signal on substantially.
The process of the electronics of the signal of telecommunication and numeral is passed through in determination to the measured variable numerical value of each sensor on FBG array
And realize, as mentioned below.
For this descriptive purpose, FBG 50 must have particular design and have the spectral response of well-characterized.
Standard FBG generally has such a reflectance spectrum, in λBCentre wavelength have reflection peak, and have side in the every side of central peak
Lobe.However, in order to realize this descriptive purpose, the height being shaped as not having minor lobe of the reflectance spectrum according to an embodiment
This function.The technology that the FBG of so gaussian-shape can be well known for those skilled in the art manufactures.For such a function,
The bandwidth △ λ of spectrumBThe wave-length coverage that reflectance is more than the 50% of maximum reflectivity can be defined as.
The effect of measured variable is to change central wavelength lambdaB.Measured variable can be temperature, strain or other change FBG
The environmental condition of the reflectance spectrum of sensor.In the measurement range formulated by sensor, spectrum will transform to maximum △ λmax.
Assume, for the light source 11 inquiring given sensor, there is wavelength XavCentered on narrow spectrum, then must set in a way
The centre wavelength of meter FBG 50 and their reflectance spectrum width, at the two ends of measurement range, FBG reflectance is sufficiently large
To lead to acceptable signal-to-interference ratio.Rule of thumb rule is it is necessary to design FBG 50 makes reflectance survey always greater than whole
The 50% of the maximum of amount scope, in this case, will select λBIt is equal to measurement span center λav, and △ λmaxEqual to △
λB.However, the reflected signal of the existing equipment illustrating is generally much higher than with reflected signal produced by broadband light source, this is public
Know, this is beneficial to be detected with high s/n ratio.
Once reflected signal changes into electronic signal, each sensor is executed with the electronics of the numerical value extracting measured variable
Can be completed by various modes known in the art with digital process.Therefore, all of achievable this process are not enumerated here
Possible mode.All these methods rely on the peak strength measuring each independent echo impulse or integral energy, and to this
Plant the application of the algorithm of measured value.According to an embodiment, the sequence of N number of pulse is by an ADC chip (analog-to-digital conversion device)
Digitized.Once by digitized, the integral energy of each echo impulse of inquiry can be by the persistent period τ related to each ripple
Temporal window signal integration calculate.Then N numerical value obtains numerical value to the pulse that each is launched, and then passes through microprocessor
Process, microprocessor can be a quick cpu chip or fpga chip, and it is programmed to perform some row steps
Process, to extract the numerical value of the measured variable of each FBG 50 in array.
This Mathematical treatment is based on following methods.As described above, the pulse being launched into optical fiber 30 has two kinds of forms, higher
Wavelength and the pulse of relatively low wavelength, respectively λ+And λ-.If having used a DFB laser diode, each type of pulse is entered
Row difference peak drive current, also by difference, respective markers are I to the peak light intensity of each pulse+And I-.Assume in light source 11
Round relay loss α and FBG 50 between keeps constant or close to constant between two kinds of forms transmittings of pulse, simultaneously
Also assume that measured variable is not changed with notable numerical value between pulse, then reflected impulse intensity is with respect to two kinds of form transmittings of pulse
Pulse strength, differ only in due to the λ in the first pulse pattern and the second pulse pattern+And λ-Different centre wavelengths lead
The difference of the reflectance causing.This is because FBG reflectance is the function of wavelength.If the FBG reflectance of the function as wavelength
Given by function R (λ), then the poor D of the peak reflection intensity of the first pulse pattern and the second pulse pattern is:
D=α * [I+*R(λ+)-I-*R(λ-)] (1)
On the other hand, intensity with S is:
S=α * [I+*R(λ+)+I-*R(λ-)] (2)
The ratio A of two amounts, is defined as A=D/S, is:
A=[I+*R(λ+)-I-*R(λ-)]/[I+*R(λ+)+I-*R(λ-)] (3)
Define ratio C=I+/ I-, then equation (3) can also be write
A=[R (λ+)-C*R(λ-)]/[R(λ+)+C*R(λ-)] (4)
It can be seen that this ratio is unrelated with propagation loss α.For constant laser drive environment, ratio C is constant, and former
It is a known quantity on then.Therefore amount A is the function of the determination of FBG reflectance spectrum R (λ) shape, numerical basis λ of AavAnd FBG
Center sensor wavelength XBDifference.If shape R (λ) is so that the function being given by equation (4) being and measurement span (spectrum window)
The monodrome of consistent span lengths, then numerical value A can uniquely draw FBG central wavelength lambdaBTwo kinds of mean wavelength λ with pulseav
Difference.Due to λavKeep constant, therefore unique variable λBRelated to measured variable.
Known ratios C, also can calculate standard value B, be given by:
B=[R (λ+)-R(λ-)]/[R(λ+)+R(λ-)] (5)
As shown below, amount B can be directly related to the derivative of the spectral shape of FBG reflectance spectrum.
Numerical value A or B is used for associating the measurement of reflected impulse intensity with measured variable.Due to following can mention former
Cause, numerical value B is preferred.
In order to explain how to realize in practice, row cite a plain example, and the shape of wherein grating spectrum is one
Gaussian function, is expressed as:
R (λ)=Rmaxexp(-4In(2)(λ+-λ-)2/△λB 2) (6)
RmaxIt is peak reflectivity, λBIt is peak wavelength, △ λBIt is the half width at half maximum of Gauss spectrum.Due to λ+With λ-difference remote
Less than spectral width △ λB, R (λ+) and R (λ -) difference close to function in wavelength XavDerivative be multiplied by λ+With λ-wavelength difference,
It is expressed as δ λ.On the other hand, the denominator in equation (5) approaches in twice in mean wavelength λavReflectance, i.e. R (λ+)+R
(λ-)=R (λav), with the function of equation 5, can draw:
B=-4In (2) Rmaxδλ(λzv-λB)2/△λB 2(7)
As can be seen that B is (λ in whole spectrumzv-λB) linear function.Other functions except the Gauss of R (λ) also may be used
To use, but they cannot derive the linear function of B.Linear feedback simplifies standard, and B is to arbitrary λBThing for monodrome
Avoid uncertain measurement in fact.Therefore, gaussian shape is effectively shape.If however, shape deviate from ideal Gaussian shape,
The existing knowledge of the spectral shape of each grating then can be used to produce calibration curve.
Numerical value B can be calculated by the peak strength of pulse or integral energy.But the latter is it is preferred that being difficult because of it
Produce noise.Further, B can averagely a large amount of pulses to reduce noise further.
In fact, ratio C can cause from pulse to pulse or produce change due to slow drift during drive electronics.
For guaranteeing with the numerical value of correct C in the numerical value calculating B, measurement is favourable in real time.This can be by direct measurement by laser
The pulse of diode emitter and realize, this be used for as FBG reflection signal normalization reference.Three kinds of sides realizing this measurement
Formula is illustrated by Fig. 6 A-C.
In first embodiment, photodiode 120 can be inserted into the outfan of photoelectrical coupler 15 second branch
(Fig. 6 A).Second is that embodiment (Fig. 6 B) is used in internal photodiode 120 in laser diode package.3rd embodiment
(Fig. 6 C) employs the reflector of fiber coupler 15 second branch's end face or any device being inserted, then by light electric-examination
Survey device 20 to detect, the same photoelectricity electroprobe of detection reflector detects the echo from sensor array 55.In latter event, must
The fiber lengths between fiber coupler and reflecting surface must be adjusted so that reflected impulse with different from other all from sensing
The time of device array echo out reaches photodiode.Detection and amplify after, these reference pulses by similarly amplify and
Digitized is to provide peak value or the comprehensive numerical value similar to echo impulse.It is similar that other equivalent embodiments are proposed that
Conclusion.
In wavelength X+N number of pulse train digitized after, can be by being carried out by the numerical value of time window to each pulse
Integrating meter calculates to the i in each sequencethThe gross energy E of pulse+i.In wavelength X+Pulse train carry out to provide E-.Identical
Process be applied to reference pulse, provide Eref+And Eref-.If in λ+Train of pulse follow in λ-Train of pulse after, then right
In each independent pulse gross energy regard train of pulse quantity meansigma methodss.So, can be extracted for each from following formula by calculating
ithThe B of pulseiN value:
Bi=((E+i/Eref+)-(E-i/Eref-))/((E+i/Eref+)+(E-i/Eref-)) (8)
As described in Fig. 3 C and 4C, wherein shadow region is equivalent to the gross energy of the first pulse in the sequence.As described above,
BiNumerical value can directly with i in an arraythThe value of the measured variable of individual FBG is related.
Modules as described above 10 can be used for autonomous device, to measure a sensor array of N number of FBG 50
55.However, having different wave length λavLight source 11 multiple modules 10, can by access single optical fiber 30, for independent inquiry
Ask multiple sensor arrays 55 of FBG 50.The spacing of the wavelength of different light sources have to be larger than spectrum window.This is divided by adopting
The output of multiple modules 10 is multiplexed to a single optical fiber 30 ripple multiplexer reaches.Light source 11 includes laser diode,
Laser diode is the type for so-called CWDM (CWDM), and it is the mark of optical telecommunications system foundation
Accurate.The wavelength of this diode, between 1270 and 1610nm, is separated with 20nm, there is provided 18 kinds of different passages.In conjunction with up to
16 passages to independent optical fiber stock for multiplexer commercially can use.Multiplexing configuration (60,65) is in figure
Illustrate in 2A.One 20nm interval is large enough to accommodate most of existing spectrum windows.The maximum capacity of therefore device 1 does not depend on
Numerical value in spectrum window.Further, standardized wavelength means that FBG 50 also has a standardized design, this fall
Low production cost.
The advantage that all light sources 11 are merged into independent optical fiber 30 is the writable light of all FBG 50
Fine 30.Therefore, along the FBG 50 of optical fiber 30 maximum quantity be the sensor inquired by each module 10 maximum number
The product of the quantity of amount and sensor 10.
But further it is an advantage that all of sensor is by the single entrance addressing to optical fiber 30, from disparate modules
10 light retargetable is to branch.For example if it is desired to measure slewing, such as multiple position measurement temperature of engine rotor
Degree or strain, then the fiber rotation connector 70 being arranged on armature spindle can be used between interrogator 12 and sensor, such as
Described in Fig. 2A.After fiber rotation connector 70, different wavelength is sent to key light by adding/deleting multiplexer
Fine corresponding branch.Such device can extract a passage (in a wavelength) and is transmitted into another optical fiber, or extracts
One group of passage.For example, 8 in 16 passages, or 4 in 8 passages are sent to individual branches, as Fig. 2A institute
State.Another embodiment according to Fig. 2 B, the fiber optic splitter being independent of wavelength can be used for the wavelength from disparate modules
More or less in the multiple optical fiber forming multiple parallel sensor arrays, each optical fiber is inquired by disparate modules for distribution.This has
The advantage that redundancy is provided, in case one of branch fault or fracture.If interrogator 12 is arranged on apart from FBG 50
When there is a big segment distance, same fibre comprises all request signals and is also advantageous.
Therefore, the modular structure of device 1 provides a lot of motilities.Various configurations for arranging FBG 50 are shown in
In Fig. 7 A-7C.Module 10 independent operation, and associated sensor array 55 all can have different characteristics, is such as passing
Different distance between sensor, or the different spectral widths of FBG 50.The latter determines measured variable scope, more determines
Determine resolution.Therefore there is large span, the sensor of low resolution can be in conjunction with the high-resolution sensor of little span.Sensor
Array 55 can be interlocked with regular spacing (Fig. 7 A), or is handed over the transducer beam of the different arrays of Small Distance binding at set intervals
Fork, this can provide higher spatial resolution (Fig. 7 B).Or other sensor arrays 55 can be linked one by one
(Fig. 7 C).The modular nature of device 1 also implies that cost increases with the module number using.Fig. 8 illustrates and adds/delete
Except how multiplexer transmits signals to corresponding branch from one or more modules 10.
DFB laser diode is made into producing 1 nanosecond or less pulse.Between therefore for sensor in an array
Minimum spacing can be as small as 10cm.The speed of electron process finally limits spacing.Because signal is lost in each reflection, sensor
Limited quantity can be used in an array, typically 15.Because up to 16 passages can be with the multiplexing that can be purchased off the shelf
Device combines, and the maximum capacity of device 1 may be up to 240 sensors.
Wavelength due to being launched by laser diode is the function of temperature, so needing the temperature control of a good diode
System 13.This available thermoelectric refrigeration element is reached, using the signal of the temperature sensor being arranged on nearly diode as an error
Signal, this is well known in the art to a certain extent.For long-time stability it is important that the central wavelength lambda of diodeav,
And two kinds of pulse wavelength difference δ λ keeps constant within the time, or if they do not keep constant, monitoring is simultaneously
Value for the scale of calibration instrument is important.It is known that laser diode degenerates with age, and therefore this two values have
May drift about in time and slowly.In order to illustrate centre wavelength and numerical value δ λ in long drift it is necessary to one by very
Good calibration stable reference sensor in known time.Reference sensor itself but to other sensors be related to similar
Fiber Bragg Grating FBG, but its temperature and strain are precisely known.This can be such as hot by with another precision temperature sensor
Quick resistance measurement FBG temperature and realize, or by keep FBG equilibrium temperature and strain other modes realize, this this
Field is known.
The performance of TDM inquiry allows such a reference sensor to inquire with the other sensors on array simultaneously.For this reason,
Sensor be necessarily placed at from inquiry unit have with a certain distance from, so from the echo with reference to grating using one of available
Time window.This is reached by the distance adjusting from source to reference sensor.Reference sensor is arranged on optical fiber coupling
Second branch of device 15, as long as in this position, on echo will fall wherein a time window.
It can be appreciated that each FBG has a known reflectance spectrum from the embodiment of foregoing description, also can claim
It is with reference to reflectance spectrum, this can offset in response to the given ambient condition using FBG 50, therefore defines to each
The skew of FBG 50.Each FBG 50 arranges different distance from light source 11 and receptor (in given array 55
Each there is interval), therefore allow to distinguish the reflection arteries and veins receiving from the FBG 50 of given array on the receptor time
Punching.
When using more than an array 55, the FBG 55 on different arrays 55 is compared with another on another array 55
One FBG 50 has same distance from light source 11 and receptor.Therefore, need spectrum point between each of array 55
From, i.e. the FBG 50 of given array 55 responds all in given spectrum window.The spectrum window characterizing different arrays 55 should not weigh
Folded.Therefore, when receiving reflected impulse, receptor can be reflected by the spectrum window of reflected impulse based on received moment and sign
Pulse, clearly defines FBG.
Due to each array 55, in the window internal reflection of given spectrum, it is therefore necessary to there is interrogator, to be adapted to transmitting such
Wavelength, this wavelength is corresponding to be given the wavelength reflection of spectrum window and avoids using broadband or tunable interrogator, as in background
Technology segment refers to.Therefore, each array 55 there is a corresponding light source 11.The described light source 11 of corresponding array adapts to
Transmitting in the spectrum window of respective array.Therefore, each array 55 and corresponding light source 11 operate in the spectrum window of each of which.
As described above, light source 11 does not need to launch in continuous wavelength scope to obtain " image " of reflected impulse, such as existing
Have performed by technology.Because the shape with reference to reflectance spectrum is known to each FBG 50, and known variant
Relatively small (less than the spectrum window of FBG 50), only has some discrete point needs in actual (skew) reflectance spectrum
It is asked.In the above-described embodiments, shape is known as (or substantially) gaussian-shape, for gaussian shape, actual (skew
) only two points need to be determined to calculate actual reflectance spectrum with respect to reference to (known) reflected light in reflectance spectrum
The change of spectrum.Accurate mensure to change, more complicated reflectance spectrums may need the wavelength of varying number.
For this reason, each light source 11 launches dispersion number not in whole spectrum window but on the corresponding spectrum window of light source 11
Wavelength (such as λ+And λ-).Due to λ+And λ-All in this spectrum window, therefore can be by defining the λ of transmitting+And λ-Between flat
All wavelength XavThis situation of formalization.Therefore, each light source 11 is characterised by the phase in the consistent corresponding spectrum window of one of array 55
Answer mean wavelength, be transmitted to the discrete wavelength of fixed number (such as 2) around it.
Received within given time and wavelength in the pulse of each FBG 50 reflection, it is used for accurately defining
The FBG 50 of reflected impulse.The actual reflectance spectrum that the pulse of reflection also reflects given FBG 50 is anti-from it
Penetrate spectral shift how many (that is, the side-play amount of each FBG 50).Therefore also reflects the main bar to FBG 50
Part.The change of each sensor 50 can be calculated, as explained above.Can be by using school in the essential condition of given sensor 50
Quasi- moving of table and be resumed.
Although embodiment is described above and is also explained by accompanying drawing, for those skilled in the art without departing from this public affairs
Substantially may make a change on the basis of opening.This change can be considered as the possible modification in open scope.
Claims (50)
1. a kind of sensor device is it is characterised in that include:
Interrogator, including light source, the transmitting of each light source has the pulse of certain wavelength, and described wavelength is around light source phase each described
The mean wavelength answered;With
FBG array, one of corresponding described light source of each FBG array, and include many on an optical fiber
The individual FBG for reflected impulse,
FBG in wherein given FBG array therebetween has a space interval, and this interval be enough in receptor
Upper permission is produced the time difference between reflected impulse by each sensor on given FBG array;
Wherein each described FBG has corresponding spectral reflectance window, and spectral reflectance window includes a corresponding described light source
Corresponding mean wavelength;
There is spectrum interval it is sufficient to allow on the receiver from each described FBG between the corresponding mean wavelength of wherein said light source
SPECTRAL DIVERSITY between the pulse of sensor array reflection.
2. sensor device according to claim 1 is it is characterised in that each described light source is configured to around described light
First respective wavelength of each the corresponding mean wavelength in source and the transmitting pulse of the second respective wavelength.
3. sensor device according to claim 1 is it is characterised in that described receptor includes processor, described place
Reason device is applied to each described FBG array of each described light source corresponding, and the reference based on each FBG
The prior art of reflectance spectrum, clearly determines each with the reflected wave pulses from the first corresponding pulses and the second corresponding pulses
The peakdeviation of the actual reflectance spectrum of FBG.
4. sensor device according to claim 1 it is characterised in that described FBG array be arranged on many
On individual optical fiber, each optical fiber has the FBG array of a given quantity.
5. sensor device according to claim 4 is it is characterised in that also include for being connected thereto multiple optical fiber
Multiplexer, described interrogator be optically coupled to multiplexer for by described pulsing to multiple optical fiber.
6. a kind of sensor device is it is characterised in that include:
Interrogator, has the light source of the pulse of certain wavelength, described wavelength is around a mean wavelength including transmitting;With
Fiber Bragg Grating FBG (FBG) configures, and including FBG array, described sensor array is included on an optical fiber
Multiple FBG, and be used for reflected impulse, thus on each FBG produce reflected impulse,
FBG on one of given FBG array betwixt has a space interval, and this space interval is connecing
Receive on device enough to allow to be produced the time difference between reflected impulse by FBG each described;
Wherein FBG array has the spectral reflectance window including described mean wavelength.
7. sensor device according to claim 6 it is characterised in that described light source be used for being transmitted in mean wavelength attached
Near first wave length and the pulse of second wave length.
8. sensor device according to claim 7 is it is characterised in that described receptor includes a processor, described
The prior art of the reference reflectance spectrum based on described multiple FBG for the processor, adaptation is with corresponding from first
The reflected impulse of wavelength and the second corresponding wavelength clearly determines the actual reflectance spectrum of each of multiple FBG.
9. a kind of device of the optical signalling interacting with Fiber Bragg Grating FBG (FBG) sensor configuration for measurement, institute
State device to include:
FBG array, sensor array is arranged along single optical fiber, and each FBG is used for operating in given spectrum window,
FBG is separated along single optical fiber with given distance, and each FBG on array has a known reflected light
Spectrum, this reflectance spectrum can be displaced in the reflectance spectrum of reality under prescribed conditions, thus defining a side-play amount;With
Interrogator, described interrogator is connected on single optical fiber and comprises module, and described module is with being included in given spectrum window
The interior discrete wavelength inquiry FBG array more than, interrogator receives the discrete wave more than of FBG
The reflection of long optical signal, to determine the side-play amount of each FBG on array.
10. device according to claim 9 it is characterised in that described module be included in given spectrum window two from
Scattered wavelength interrogation FBG array.
11. devices according to claim 10, it is characterised in that the described given distance that is spaced of FBG, lead to
Time difference between the reflection of optical signalling that described interrogator receives.
, it is characterised in that also including a processor, described processor is operable for 12. devices according to claim 11
Be connected to interrogator, and be adapted to execute instruction for determining the instruction of specified criteria, under to described fixed condition it is known that
Reflectance spectrum is displaced in the reflectance spectrum of each FBG reality on array.
A kind of 13. devices of the optical signalling interacting with Fiber Bragg Grating FBG (FBG) sensor configuration for measurement, its
It is characterised by, described device includes:
Multiple FBG tactility apparatus arrays, sensor array is arranged along the multiple optical fiber branching out in main fiber, the plurality of array
Each FBG having different spectrum windows and including operation in difference spectrum window, described FBG has one
Known reflectance spectrum, this spectrum can experience skew in specified criteria, therefore defines side-play amount to each FBG;
Interrogator, is connected on main fiber and includes multiple modules, and each module uses an array of corresponding FBG not
With the array of a FBG corresponding more than the pulse interrogation of in spectrum window, interrogator receives and is reflected by FBG
And indicate the optical signalling of the side-play amount of each FBG.
14. devices according to claim 13 are it is characterised in that each module uses the array of corresponding FBG
The pulse more than one of interior different spectrum windows, inquires the array of corresponding FBG, clearly to evaluate each FBG biography
The side-play amount of the known reflectance spectrum of sensor.
15. devices according to claim 13 are it is characterised in that the FBG of described given array is along multiple optical fiber
One of separated with given distance, on optical fiber, FBG is configured to:When optical signalling is reflected by FBG, energy
Enough produce the time difference of described optical signalling pulse.
16. devices according to claim 13, it is characterised in that also including a multiplexer, are arranged on interrogator
And multiple array between, multiplexer is used for for the output of multiple modules integrating with main fiber.
17. one kind are used for measuring the device of the optical signalling of Fiber Bragg Grating FBG (FBG) sensor configuration, described device bag
Include:
Along the array of the FBG of single optical fiber setting, each described FBG has to be centered around and moves under change condition
Peak reflectance wavelength known reflectance spectrum:With
Interrogator, described interrogator is connected to independent optical fiber and includes:
Module, is adapted to inquire the array of FBG using optical signalling, described optical signalling is with first wave length (λ+) or the
Two wavelength (λ-) transmitting pulse;With
Receptor, to detect the pulse reflected by FBG array, i.e. reflected impulse, for determining at least one for adaptation
The side-play amount of the peak reflectance wavelength of individual FBG.
18. devices according to claim 17 are it is characterised in that the additional FBG also including being arranged at additional optical fiber passes
The array of sensor, the array of each additional FBG has different and unique peak reflectance wavelength;Described inquiry
Device also includes additional module, is adapted to the array of the FBG additional with different optical signalling inquiries, described optical signalling
Including with first wave length (λ+) or second wave length (λ-) pulse launched, wherein λ+And λ-For each additional module
It is different and unique.
19. devices according to claim 17, it is characterised in that described receptor includes a photodiode, are used
In optical signalling being changed into the electronic signal representing described optical signalling.
20. devices according to claim 19, it is characterised in that described receptor includes an amplifier, are used for putting
Described greatly electronic signal.
21. devices according to claim 20 are it is characterised in that described receptor is for defeated with the described receptor of process
The processing meanss operation communication of the electronic signal going out.
22. devices according to claim 21 it is characterised in that side-play amount based on peak reflectance wavelength, fit by processor
Be made into by locate reason receptor output electronic signal determine act on measured at least one FBG.
23. devices according to claim 22 are it is characterised in that described processing equipment is adapted to for determining in effect
At least one of temperature at least one sensor and strain.
It is characterised in that also including swivel joint, described swivel joint is set 24. devices according to claim 17
It is placed between interrogator and described single optical fiber, be used for making single optical fiber rotate with respect to described interrogator.
It is characterised in that described interrogator includes light source, described light source includes swashing 25. devices according to claim 17
Optical diode.
26. devices according to claim 25 it is characterised in that also including cooling element, for keeping described light source
Temperature.
27. devices according to claim 26 are it is characterised in that described cooling unit includes the cooling unit of thermoelectricity.
28. devices according to claim 26 it is characterised in that also including temperature sensor, for measuring the temperature of light source
Degree, and and then notify whether described cooling element is necessary to cool down described light source.
29. devices according to claim 25 are it is characterised in that also include the reference laser for monitoring described optical signal
Diode.
30. devices according to claim 29 are it is characterised in that described reference laser diode is described in order to monitor
The long-term wave length shift of light source.
31. devices according to claim 29 are it is characterised in that also include photo-coupler, for launch slave module
Pulse steering configures to FBG and from described FBG sensing configuration, reflected impulse is directed to described receptor, described
Photo-coupler there is the second branch, wherein said reference photodiode is arranged on the second branch of described photo-coupler
On.
32. devices according to claim 17 it is characterised in that also including photo-coupler, for sending out from described module
The pulse steering penetrated is to described FBG configuration, and described reflected impulse is directed to from the configuration of described FBG
Described receptor.
A kind of 33. optical signallings being reflected by Fiber Bragg Grating FBG (FBG) sensing device including FBG for measurement
Method, the method comprising the steps of:
Configure to described FBG from a light source and send:
At least one pulse in first wave length;With
In at least one pulse of second wave length,
Each pulse is at least separated with time interval T, and each pulse is shorter than unit interval T, passes from each FBG for difference
The reflected impulse of sensor;
For at least one FBG, receive and measure following intensity:
Reflected impulse at least one pulse of first wave length;With
In the reflected impulse of at least one pulse of second wave length,
Calculate the peak reflectance wavelength of at least one described FBG.
34. methods according to claim 33 receive and measurement intensity it is characterised in that being executed by receptor.
35. methods according to claim 34 it is characterised in that described receptor be adapted to sufficiently fast response with
So that distinguishing the reflected impulse from each sensor.
36. methods according to claim 34 are it is characterised in that described time interval T is from adjacent FBG
The time interval that received on described receptor of reflected impulse.
37. methods according to claim 33 are it is characterised in that also include determining described peak reflectance wavelength with respect to institute
State the side-play amount of the reference value of peak reflectance wavelength.
38. methods according to claim 37 are it is characterised in that also include being gone with the side-play amount of described peak reflectance wavelength
Determine the value of the measured variable acting at least one FBG.
39. methods according to claim 33 are it is characterised in that also include with light source described in reference laser diode monitor
Wavelength.
40. methods according to claim 39 are it is characterised in that also include using independent temperature sensor measurement reference
The temperature of laser diode.
41. methods according to claim 40 are it is characterised in that also include controlling the temperature of described light source.
42. methods according to claim 41 are it is characterised in that control the temperature of light source to include:Cooling unit with thermoelectricity
The described light source of part cooling.
43. methods according to claim 42 are it is characterised in that the temperature controlling light source is based on from temperature sensor
Input, whether the temperature of described temperature sensor measurement light source deviates particular value.
44. methods according to claim 33 it is characterised in that be sent at least one of first wave length with the first intensity
Pulse, is sent at least one pulse of second wave length with the second intensity, and the intensity of wherein measurement reflected impulse includes detection often
The disappearance of individual pulse respective strengths.
45. methods according to claim 33 it is characterised in that to described FBG configure send pulse include to
The FBG being arranged on multiple optical fiber sends.
A kind of 46. methods of Fiber Bragg Grating FBG (FBG) sensor configuration comprising FBG for inquiry, described side
Method comprises the following steps:
FBG array to FBG configuration sends multiple optical signals, and each described optical signal is used for and single FBG array
On the interaction of described FBG, each optical signal includes:
At least one pulse of corresponding first wave length;With
At least one pulse of corresponding second wave length,
Each corresponding mean wavelength of described optical signals is to characterize, corresponding first and second ripples in each optical signal described
Length provides around described mean wavelength:
For at least one FBG of FBG array, receive and measure following intensity:
Reflected impulse at least one pulse of described first wave length;With
Reflected impulse at least one pulse of described second pulse;And
To FBG at least one described, calculate peak reflectance wavelength.
47. methods according to claim 46 are it is characterised in that to each optical signal, each pulse is at least spaced accordingly
Time interval T, wherein each pulse is shorter than corresponding time interval T.
48. methods according to claim 46 receive and measurement intensity it is characterised in that being executed by receptor, described
Receptor response sufficiently fast so that the reflected impulse from each FBG can be distinguished.
49. methods according to claim 46 are it is characterised in that each FBG array has following characteristics:In each FBG
On array, all FBG of setting share corresponding spectrum window, and each FBG array is ask with a corresponding optical signalling
Ask.
50. methods according to claim 49 are it is characterised in that corresponding mean wavelength in each described optical signalling
Between, there is the spectrum accordingly composing window more than each FBG array and separate, enabling spectrum difference is carried out to each FBG array.
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US201461973975P | 2014-04-02 | 2014-04-02 | |
US61/973,975 | 2014-04-02 | ||
PCT/CA2015/000232 WO2015149162A1 (en) | 2014-04-02 | 2015-04-02 | Apparatus for measuring optical signals from multiple optical fiber sensors |
Publications (2)
Publication Number | Publication Date |
---|---|
CN106471340A true CN106471340A (en) | 2017-03-01 |
CN106471340B CN106471340B (en) | 2019-07-23 |
Family
ID=54209515
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201580030292.6A Active CN106471340B (en) | 2014-04-02 | 2015-04-02 | For the device from multiple fiber sensor measuring optical signals |
Country Status (3)
Country | Link |
---|---|
US (1) | US9810556B2 (en) |
CN (1) | CN106471340B (en) |
WO (1) | WO2015149162A1 (en) |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110785666A (en) * | 2017-04-06 | 2020-02-11 | 斯奈普泰克有限公司 | Multi-phase sensor module, system and method |
CN112105894A (en) * | 2018-04-09 | 2020-12-18 | 基德科技公司 | Device for monitoring a measured quantity |
CN112595253A (en) * | 2020-11-10 | 2021-04-02 | 新疆大学 | Surface strain dynamic optical fiber grating detection device |
CN113218428A (en) * | 2021-05-25 | 2021-08-06 | 成都大学 | Fiber grating sensor measuring system with traceable calibration function |
WO2023004760A1 (en) * | 2021-07-30 | 2023-02-02 | F·欧莱特 | Temperature-compensating optical fiber strain gauge with variable range |
Families Citing this family (17)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9551809B2 (en) * | 2015-02-04 | 2017-01-24 | Baker Hughes Incorporated | Arrayed wave division multiplexing to improve spatial resolution of IOFDR fiber Bragg sensing system |
GB201503861D0 (en) | 2015-03-06 | 2015-04-22 | Silixa Ltd | Method and apparatus for optical sensing |
EP3291192A1 (en) * | 2016-09-01 | 2018-03-07 | Airbus Operations, S.L. | Monitoring system of an aircraft bleed air system |
CN106525091A (en) * | 2016-10-25 | 2017-03-22 | 华中科技大学 | Fiber grating array sensing demodulation system based on multi-wavelength pulse differential modulation |
WO2018089831A1 (en) * | 2016-11-10 | 2018-05-17 | Ryan Seeley | Optical sensor and systems and methods |
US10895692B2 (en) * | 2017-06-01 | 2021-01-19 | Canon U.S.A., Inc. | Fiber optic rotary joints and methods of using and manufacturing same |
WO2019027854A1 (en) | 2017-08-01 | 2019-02-07 | Schlumberger Technology Corporation | Simultaneous distributed measurement monitoring over multiple fibers |
CN107894516A (en) * | 2017-09-05 | 2018-04-10 | 南京牧镭激光科技有限公司 | A kind of calibration system of the range gate of laser radar |
GB2570144A (en) * | 2018-01-12 | 2019-07-17 | Ap Sensing Gmbh | High rate fibre optical distributed acoustic sensing |
GB2571575B (en) * | 2018-03-02 | 2022-05-04 | Univ Cranfield | An optical shape sensing method and system |
US10768055B2 (en) * | 2018-03-06 | 2020-09-08 | Kidde Technologies, Inc. | Device and method of calibrating fiber Bragg grating based fiber optic overheat systems |
DE102018107162A1 (en) * | 2018-03-26 | 2019-09-26 | Nkt Photonics Gmbh | sensor system |
US10797789B2 (en) * | 2018-06-28 | 2020-10-06 | Nec Corporation | Distributed fiber sensing interrogator with detachable end |
CN112834072B (en) * | 2021-02-08 | 2021-09-24 | 广东海洋大学 | Michelson interference optical fiber temperature sensor for detecting stripe contrast change |
CN113155165B (en) * | 2021-05-14 | 2022-07-05 | 武汉理工大学 | Interference type demodulation system and method for large-capacity fiber grating sensor network |
WO2023186229A1 (en) * | 2022-03-28 | 2023-10-05 | Vestas Wind Systems A/S | Wind turbine with control network and monitoring network |
US20230344544A1 (en) * | 2022-04-22 | 2023-10-26 | Halliburton Energy Services, Inc. | Fiber Optic Sensing And Communication Systems |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5757487A (en) * | 1997-01-30 | 1998-05-26 | The United States Of America As Represented By The Secretary Of The Navy | Methods and apparatus for distributed optical fiber sensing of strain or multiple parameters |
US5991026A (en) * | 1996-03-11 | 1999-11-23 | Sensor Dynamics Limited | Apparatus for multiplexing fibre-optic sensing interferometers |
US20050269489A1 (en) * | 2004-06-04 | 2005-12-08 | Domino Taverner | Optical wavelength determination using multiple measurable features |
US20110181871A1 (en) * | 2010-01-28 | 2011-07-28 | Baker Hughes Incorporated | Combined swept-carrier and swept-modulation frequency optical frequency domain reflectometry |
CN103454014A (en) * | 2012-05-31 | 2013-12-18 | 基德科技公司 | Optical fiber sensing system |
CN103460008A (en) * | 2011-02-09 | 2013-12-18 | 西门子能量股份有限公司 | Multiplexed optical fiber wear sensor |
Family Cites Families (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6571027B2 (en) * | 1999-10-07 | 2003-05-27 | Peter W. E. Smith | Method and devices for time domain demultiplexing of serial fiber bragg grating sensor arrays |
US20040046109A1 (en) | 2002-09-05 | 2004-03-11 | Chen Peter C. | Method and apparatus for high speed interrogation of fiber optic detector arrays |
US7119325B2 (en) * | 2003-01-27 | 2006-10-10 | Bookham Technology Plc | System and method for monitoring environmental effects using optical sensors |
US7127132B1 (en) * | 2004-03-08 | 2006-10-24 | Ifos, Inc. | Cascade fiber-optic grating-based sensor apparatus and method |
FR2889305B1 (en) | 2005-07-28 | 2007-10-19 | Sercel Sa | FIBER OPTIC INTERFEROMETER NETWORK |
US7995209B2 (en) | 2008-10-06 | 2011-08-09 | Schlumberger Technology Corporation | Time domain multiplexing of interferometric sensors |
GB2464477B (en) * | 2008-10-15 | 2011-09-07 | Insensys Ltd | Apparatus for interrogating fibre Bragg gratings |
IN2014DN03226A (en) * | 2011-09-30 | 2015-05-22 | Vestas Wind Sys As | |
JP5628779B2 (en) * | 2011-12-01 | 2014-11-19 | 株式会社日立製作所 | Multipoint measuring method and multipoint measuring apparatus for FBG sensor |
US9389174B2 (en) * | 2014-06-18 | 2016-07-12 | Weatherford Technology Holdings, Llc | Time division multiplexing (TDM) and wavelength division multiplexing (WDM) sensor arrays |
-
2015
- 2015-04-02 US US14/677,470 patent/US9810556B2/en active Active
- 2015-04-02 WO PCT/CA2015/000232 patent/WO2015149162A1/en active Application Filing
- 2015-04-02 CN CN201580030292.6A patent/CN106471340B/en active Active
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5991026A (en) * | 1996-03-11 | 1999-11-23 | Sensor Dynamics Limited | Apparatus for multiplexing fibre-optic sensing interferometers |
US5757487A (en) * | 1997-01-30 | 1998-05-26 | The United States Of America As Represented By The Secretary Of The Navy | Methods and apparatus for distributed optical fiber sensing of strain or multiple parameters |
US20050269489A1 (en) * | 2004-06-04 | 2005-12-08 | Domino Taverner | Optical wavelength determination using multiple measurable features |
US20110181871A1 (en) * | 2010-01-28 | 2011-07-28 | Baker Hughes Incorporated | Combined swept-carrier and swept-modulation frequency optical frequency domain reflectometry |
CN103460008A (en) * | 2011-02-09 | 2013-12-18 | 西门子能量股份有限公司 | Multiplexed optical fiber wear sensor |
CN103454014A (en) * | 2012-05-31 | 2013-12-18 | 基德科技公司 | Optical fiber sensing system |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110785666A (en) * | 2017-04-06 | 2020-02-11 | 斯奈普泰克有限公司 | Multi-phase sensor module, system and method |
CN110785666B (en) * | 2017-04-06 | 2023-02-17 | 斯奈普泰克有限公司 | Multi-phase sensor module, system and method |
CN112105894A (en) * | 2018-04-09 | 2020-12-18 | 基德科技公司 | Device for monitoring a measured quantity |
US11549829B2 (en) | 2018-04-09 | 2023-01-10 | Kidde Technologies, Inc. | Apparatus for monitoring a measurand |
CN112595253A (en) * | 2020-11-10 | 2021-04-02 | 新疆大学 | Surface strain dynamic optical fiber grating detection device |
CN113218428A (en) * | 2021-05-25 | 2021-08-06 | 成都大学 | Fiber grating sensor measuring system with traceable calibration function |
WO2023004760A1 (en) * | 2021-07-30 | 2023-02-02 | F·欧莱特 | Temperature-compensating optical fiber strain gauge with variable range |
Also Published As
Publication number | Publication date |
---|---|
WO2015149162A1 (en) | 2015-10-08 |
CN106471340B (en) | 2019-07-23 |
US20150285683A1 (en) | 2015-10-08 |
US9810556B2 (en) | 2017-11-07 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN106471340B (en) | For the device from multiple fiber sensor measuring optical signals | |
US6680472B1 (en) | Device for measuring of optical wavelengths | |
CN1726664B (en) | Optical interrogation system and sensor system | |
US6449047B1 (en) | Calibrated swept-wavelength laser and interrogator system for testing wavelength-division multiplexing system | |
US7573021B2 (en) | Method and apparatus for multiple scan rate swept wavelength laser-based optical sensor interrogation system with optical path length measurement capability | |
US5838437A (en) | Reference system for optical devices including optical scanners and spectrum analyzers | |
Dai et al. | A novel time-division multiplexing fiber Bragg grating sensor interrogator for structural health monitoring | |
US8005323B2 (en) | Method and apparatus for generation and transmission of high energy optical pulses for long range measurements | |
US9958300B2 (en) | Time division multiplexing (TDM) and wavelength division multiplexing (WDM) fast-sweep interrogator | |
CN100507455C (en) | Intensity modulation type optical fiber sensor multiplexing method | |
CN108880668A (en) | A kind of railway optical cable real-time monitoring system for state and method | |
CN101517375A (en) | Measuring brillouin backscatter from an optical fibre using channelisation | |
KR20010074858A (en) | Method and apparatus for optical performance monitoring in wavelength division multiplexed fiber optical systems | |
CN101523183A (en) | Measuring Brillouin backscatter from an optical fibre using a tracking signal | |
Lloyd et al. | Resonant cavity time-division-multiplexed fiber Bragg grating sensor interrogator | |
EP0727640B1 (en) | Optical distance measurement | |
CN102818531A (en) | Dynamic strain measurement instrument based on multiple overlapped gratings | |
CN1963399A (en) | Multiplex fibre optic interferometer and nesting constructing method of the same | |
CN105806374B (en) | A kind of demodulation method of optic fiber grating wavelength | |
CN109000694A (en) | Grating prepares on-line monitoring method and system | |
EP0932814B1 (en) | An optical wavelength scanner employing a reference system | |
JP4625593B2 (en) | Optical fiber multipoint physical quantity measurement system | |
KR101752853B1 (en) | Sensor device | |
WO2023148357A1 (en) | Measurement device and measurement method | |
Dai et al. | Fiber Bragg grating sensor multiplexing system based on the time-and wavelength-division technique |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant | ||
TR01 | Transfer of patent right |
Effective date of registration: 20200914 Address after: Quebec Patentee after: F. Ollett Address before: Quebec Patentee before: KROMASENSE Inc. |
|
TR01 | Transfer of patent right |